EP0335468A1 - Electro-acoustical system - Google Patents
Electro-acoustical system Download PDFInfo
- Publication number
- EP0335468A1 EP0335468A1 EP89200785A EP89200785A EP0335468A1 EP 0335468 A1 EP0335468 A1 EP 0335468A1 EP 89200785 A EP89200785 A EP 89200785A EP 89200785 A EP89200785 A EP 89200785A EP 0335468 A1 EP0335468 A1 EP 0335468A1
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- Prior art keywords
- loudspeaker
- sound
- microphone
- hall
- ijk
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- G—PHYSICS
- G10—MUSICAL INSTRUMENTS; ACOUSTICS
- G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
- G10K15/00—Acoustics not otherwise provided for
- G10K15/08—Arrangements for producing a reverberation or echo sound
- G10K15/12—Arrangements for producing a reverberation or echo sound using electronic time-delay networks
-
- G—PHYSICS
- G10—MUSICAL INSTRUMENTS; ACOUSTICS
- G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
- G10K15/00—Acoustics not otherwise provided for
- G10K15/02—Synthesis of acoustic waves
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04S—STEREOPHONIC SYSTEMS
- H04S7/00—Indicating arrangements; Control arrangements, e.g. balance control
- H04S7/30—Control circuits for electronic adaptation of the sound field
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04S—STEREOPHONIC SYSTEMS
- H04S7/00—Indicating arrangements; Control arrangements, e.g. balance control
- H04S7/30—Control circuits for electronic adaptation of the sound field
- H04S7/307—Frequency adjustment, e.g. tone control
Definitions
- This preprint introduces a generalized description of electro-acoustical systems designed to improve the reproduction of sound in a room or, in other terms, to change or improve the accoustic conditions in a listening room.
- Dependent on the location of the microphones S represents direct sound, reflected sound, or both.
- Dependent on the purpose of the electro-acoustica system P represents direct sound, reflected sound, or both.
- the working of an electro-acoustical system is determined by the selection of the elements in the transfer matrix T.
- the above preprint does not teach how to make such selection.
- ⁇ nm represents the delay between microphone m and loudspeaker n
- a nm ( ⁇ ) represents the frequency dependent amplification (or attenuation) between microphone m and loudspeaker n.
- a more advanced PA system with a mixing console and e.g. six microphones and two loudspeakers, can be represented by
- very early reflections may be generated to support the direct sound, such as applied in so-called "Delta-stereofonie” (vide W. Ahnert: The Complex Simulation of Acoustical Sound Fields by the Delta Stereophony System (DSS), 81 st Convention of the Audio Engineering Society, J. Audio Eng. Soc. (Abstracts), vol. 34, p.1035, December 1986).
- DSS Delta Stereophony System
- the delay ⁇ nm is selected such, that the sound of loud speaker n reaches the listener not earlier, and not later either than a few dozens of ms after the natural direct sound.
- Reflection generating systems add to each direct sound microphone signal a desired reflection by selecting the amplitudes and delays of the matrix elements according to the ray paths.
- the invention aims at improving the above well-known methods such that optimum acoustical conditions are obtained for any source position on the stage and any listener position in any given listening room.
- the measures proposed by the present invention involve the application of the principle of the acoustical holography or wave field extrapolation, described in chapters VIII and X of the book "Applied Seismic Wave Theory" by A.J. Berkhout, Edition Elsevier, 1987.
- Wave field extrapolation has brought substantial progress in the field of exploration seismics. This progress has been possible also thanks the application of holographic techniques, whereby seismic wave fields, measured by seismometers on the earth surface, are extrapolated according to geologic structures on great depth.
- the invention is thus based on the surprising insight that the above principles may be advantageously transferred to the field of electro-acoustics.
- the application of the holographic principle implies an approach of the above sound transfer problem according to the wave theory, in contrast with the approach according to the ray theory in e.g. EP 0075615, in which only a marginal improved sound reproduction in a small portion of the total listening area is achieved.
- the invention also relates to an electro-acoustical system comprising means for carrying out the method above described.
- noise-suppressing filters for the attenuation of acoustical noise.
- the electro-acoustical system according to the invention permits the acoustical conditions in multi-functional halls to be adjusted in a flexible manner in accordance with the specific use, while as much freedom as possible is left to the architect.
- the system according to the invention enlarges the possibilities for both the architect and the acoustician.
- the acoustician determines the pattern of the reflections of the order zero, one and higher, which would exist in a fictive hall and which would be ideal for a certain use. These desired, natural, spatial reflection patterns are generated by a configuration of microphones and loudspeakers in the existing room.
- the unique situation is created that in the existing hall designed by the architect, that acoustic condition can be realized which fits with a fictive ideal hall in accordance with the choice of the acoustician.
- the acoustical parameters such as volume, volume, form and absorption of the fictive hall, the acoustic condition in the existing room changes in a very natural manner.
- the reverberation time may be substantially lengthened without the danger of colouring, whereas the reverberation level may be changed independent of the reverberation time - even such that both 'single-decay' and 'double-decay' curves may be achieved.
- lateral reflections may be extra emphasized and the direct field may be substantially amplified in a very natural manner, i.e. without localisation errors.
- acoustical noise may be reduced by:
- a major advantage of the system according to the invention is to be seen in that fine-tuning from the real room is possible, as a re suit of which each desired sound field may be almost completely achieved.
- the electro-acoustical system according to the present invention may be realised in eight steps:
- Each parameter may be varied in steps.
- the advantage of the above measures is to be seen in that the fading in of the system may be effected in a quick and simple manner and that each objective and subjective demand can be met.
- the system according to the invention may be composed of three parts:
- the central processor embodies the transfer matrix T and forms the heart of the electro-acoustical system.
- each reflection simulating unit is taking care of a weighed and delayed signal between each microphone and each loudspeaker.
- the various reflection simulating units are internally coupled. The required number of units depends on the size and the form of the room and the required maximum reverberation time.
- the system according to the invention may consist of any combination of four independent modules, viz. a hall module, a stage module, a speech module and a theatre module.
- this module By means of this module a desired reverberation field may be realised in the hall, tending to maximum "spaciousness". In halls with deep balconies it will often be necessary to use a number of reverberation modules. Early reflections may be additionally amplified or late reflections may be additionally attenuated to improve the 'definition' of music. By means of the system according to the invention it is even possible to have sound decay at two rates, e.g. at first quick and then slow.
- this module By means of this module the early reflections desired on the stage may be realised, thereby creating optimum combined action conditions for the musicians of an ensemble.
- PA public address
- the direct sound field reflections of the order zero
- the direct sound field may be reconstructed in any spot of the room in a completely natural manner, i.e. keeping the correct localisation and in each frequency band with any desired level.
- This module is speech supporting by adding early reflections without making use of PA-microphones: the direct sound is picked up by a number of microphones over and/or in front of the stage. Reconstruction is taking place as with the speech module.
- the sound is reverberated. Thereupon the reverberation sound field is picked up by receivers, such as receiver 8 and transmitted to corresponding locations 9 in the real architectonic room 5 by means of loudspeakers, such as loudspeaker 9.
- Source 13 in the desired hall 7 has the same position as the microphone 6 in the real room 5.
- the receiver 8 in the desired hall 7 has the same position as the loudspeaker 9 in the real hall 5.
- an acoustically ideal hall may be 'constructed' within the architectonic hall.
- the acoustical system according to the present invention can be considered to work with two halls: the real hall and a fictive one.
- Said one microphone-loudspeaker pair in fig. 2 only serves to illustrate the transfer action or - processing, which is taking place between a microphone and a loudspeaker via reproduction - and pick up components in the fictive hall.
- the type of transfer aimed at by the invention required a dense network of microphones and loudspeakers, so that a wave field may be created both on the input and the output side. It has been found that by means of linear-y arrays of loudspeakers at the side walls and ceilings with a mutual spacing of about 2 m very good results may be obtained.
- Fig. 4 illustrates the system according to the invention in block diagram for one microphone-loudspeaker pair.
- the processor 15 may operate either in the analog or in the digital mode.
- the feedback phenomenon (quantified by G nm ) may be minimized, viz. to
- R m n ( ⁇ ) ⁇ R mn ( ⁇ ) is aimed at.
- a compensation circuit comprising an noise-suppressing filter may be additionally applied according to where I indicates the microphone position adjacent the noise source, such as a tan opening.
- the data flow has been shown in diagrammatic form.
- the source wave field is picked up by a network of microphones 20.
- the desired reflection pattern - belonging to the fictive hall 7 - is simulated by the central processor T.
- Said reflection pattern is then transmitted to the real hall 5 by means of a network of loudspeakers 10.
- Fig. 6 shows a diagrammatic configuration of a reflection-simulating unit 16 (order zero for speech, first and higher order for reverberation). The coefficients are determined in the manner indicated above.
- the central processor T comprises a number of reflection simulating units 16. Each reflection simulating unit is determined by the transfer function between M sources 11 and N loudspeakers 12 for a certain order of reflection.
- the relation between input and output may be represented by a transfer matrix T (“transfer”) as follows:
- the transfer matrix T is designed per octave band and is thus composed of a number of submatrices: Tijk
- i is the number of reflections against the side walls
- j is the number of reflections against front and back walls
- k is the number of reflections against ceiling and floor.
- the source factor S is composed of a number of sub-factors S ; jk .
- Fig. 8 illustrates the simulation of the desired reverberation field, by using the image source approach.
- Each simulating unit represents the transfer function between the sources in one image version of the fictive hall and the loudspeaker in the real hall.
- a reference setting is determined by carrying out interactive measurements such that T so values and sound pressure levels meet the specifications.
- the reference setting could be selected such that, when the system is switched on, the reverberation time values in octave bands measured in the hall correspond to those in the Amsterdam Concertgebouw, with reverberant sound pressure levels related to the reverberation times according to physical laws.
- appropriate ratios of early-to-late and lateral-to-frontal energy could be aimed at.
- preference settings can be adjusted to 'instantaneous multi-purpose requirements' or 'subjective alternatives' by varying 19 fine-tuning parameters:
- Fig. 12 and 13 show a few decay curves, applying for the auditorium of the Delft University ('single decay') and the York University ('double decay') respectively for 500 Hz. It will be appreciated, that very small decay rates may be generated without the slightest tendency to colouring. It has been found that settings with relatively strong early reflections (or relatively weak late-reflections) create an excellent intelligibility, even with reverberation times of as high as 4s.
Abstract
A method and acoustical system for processing sound signals according to the principle of the acoustic holography or sound wave field extrapolation.
Description
- The invention relates to a a method and electro-acoustical system for processing the sound emitted by one or more sound sources in a listening room, by recording said sound by means of a number of microphones, the signals (S) of which are processed in a processor according to the matrix relation P = T S , in which (P) represents the processed signals supplied from the processor to a number of loudspeakers distributed across the listening room, and wherein T represents the following transfer matrix:
- This preprint introduces a generalized description of electro-acoustical systems designed to improve the reproduction of sound in a room or, in other terms, to change or improve the accoustic conditions in a listening room. This description is based on the consideration that each lineary transfer, whereby sound is picked up by microphones (S) and, after being processed, is emitted by loudspeakers (P), can be represented by the above matrix relation
P = TS . Dependent on the location of the microphonesS represents direct sound, reflected sound, or both. Dependent on the purpose of the electro-acoustica systemP represents direct sound, reflected sound, or both. - The working of an electro-acoustical system is determined by the selection of the elements in the transfer matrix T. The above preprint does not teach how to make such selection.
- A complete development of the relation
P = TS results in: -
- A number of well-known electro-acoustical systems will now be considered in the light of the above general matrix notation:
- 1. In a so-called 'public address' (PA) system the microphones are located close to the sound source and they largely pick up the direct sound. They delays are generally zero. For a simple single channel PA system M = N = 1, τ11 = 0 and A11 (ω) equals the desired frequency dependent amplification, P1 = All (ω) Si.
-
- 2. In reverberation enhancement systems, such as the well-known MCR system of Phillips, the microphones largely pick up the reverberant sound field, which means that Si, S2 ........ SM principally define reverberant sound signals (vide Fransen, N.V.; Sur amplification des champs Acbustiques, Acoustica vol. 18, pp 315 -223 (1968)). Moreover, the transfer coefficience are delay-free and τnm (ω) = Anm (ω) represents the frequency dependent channel amplification between microphone m and loudspeaker n. Microphones and loudspeakers that are located close to another must have very small (or zero) amplification to avoid colouration or even hawl-back. An optimum choice of all Anm (ω) values, such that enough reverberant energy is generated on the one hand and colouration is avoided on the other hand, is difficult and requires many channels.
- 3. In reflection generation systems, such as the system disclosed in EP 0075615, the response can be described by the above matrix relation, with a diagonal matrix
- As a special example, very early reflections may be generated to support the direct sound, such as applied in so-called "Delta-stereofonie" (vide W. Ahnert: The Complex Simulation of Acoustical Sound Fields by the Delta Stereophony System (DSS), 81 st Convention of the Audio Engineering Society, J. Audio Eng. Soc. (Abstracts), vol. 34, p.1035, December 1986).
- In this system the delay τnm is selected such, that the sound of loud speaker n reaches the listener not earlier, and not later either than a few dozens of ms after the natural direct sound.
- Reflection generating systems add to each direct sound microphone signal a desired reflection by selecting the amplitudes and delays of the matrix elements according to the ray paths.
- These systems are thus based on ray theory, which means that the desired reflection sequence can be optimally designed only for one specific source and receiving position. As a result of this the solutions embodies in these systems apply, in principle, for a small listening area only. Moreover, if the source position changes, the coefficient τnm has to be adjusted (n = 1, 2 ....... N).
- The invention aims at improving the above well-known methods such that optimum acoustical conditions are obtained for any source position on the stage and any listener position in any given listening room.
- According to the invention this aim is achieved in that the microphone array is arranged to pick up the wave field of the direct sound originating from all of the sources on the stage, the elements of the matrix T being selected according to the Green's function in the Kirchhoff-integral
- In a similar way, according to a further characteristic of the invention, sound wave fields which are (additionally) based on (very) early end/or late' reflections (reverberant sound) may be simulated by (additionally) processing the picked up direct sound signals according to the matrix relation
S ijk represent the image sources in the acoustically desired image hall (i, j, k) and Tijk represent the Kirchhoff-based transfer matrix of the image sources in the image hall (i, j, k) to the loudspeakers in the real listening room and where for the image sourcesS ijk = (1 - aijk)S applies, where aijk represents the total absorption after (i + j + k) reflections. - It will be understood that for simulating the direct sound field, the real position of each microphone has to be taken into consideration, while for simulating of reflected wave fields the mirror images of the microphone positions in the acoustically desired hall have to be considered.
- The measures proposed by the present invention involve the application of the principle of the acoustical holography or wave field extrapolation, described in chapters VIII and X of the book "Applied Seismic Wave Theory" by A.J. Berkhout, Edition Elsevier, 1987.
- Wave field extrapolation has brought substantial progress in the field of exploration seismics. This progress has been possible also thanks the application of holographic techniques, whereby seismic wave fields, measured by seismometers on the earth surface, are extrapolated according to geologic structures on great depth. The invention is thus based on the surprising insight that the above principles may be advantageously transferred to the field of electro-acoustics.
- The application of the holographic principle implies an approach of the above sound transfer problem according to the wave theory, in contrast with the approach according to the ray theory in e.g. EP 0075615, in which only a marginal improved sound reproduction in a small portion of the total listening area is achieved.
- The invention also relates to an electro-acoustical system comprising means for carrying out the method above described.
- In order to combat the influence of sound sources, such as fans, use may be made of noise-suppressing filters for the attenuation of acoustical noise.
- The electro-acoustical system according to the invention permits the acoustical conditions in multi-functional halls to be adjusted in a flexible manner in accordance with the specific use, while as much freedom as possible is left to the architect. The system according to the invention enlarges the possibilities for both the architect and the acoustician. The acoustician determines the pattern of the reflections of the order zero, one and higher, which would exist in a fictive hall and which would be ideal for a certain use. These desired, natural, spatial reflection patterns are generated by a configuration of microphones and loudspeakers in the existing room. By means of the system according to the invention the unique situation is created that in the existing hall designed by the architect, that acoustic condition can be realized which fits with a fictive ideal hall in accordance with the choice of the acoustician. By changing the acoustical parameters, such as volume, volume, form and absorption of the fictive hall, the acoustic condition in the existing room changes in a very natural manner.
- Due to the fact that the system according to the invention is not based on acoustical feedback, the reverberation time may be substantially lengthened without the danger of colouring, whereas the reverberation level may be changed independent of the reverberation time - even such that both 'single-decay' and 'double-decay' curves may be achieved. Moreover, lateral reflections may be extra emphasized and the direct field may be substantially amplified in a very natural manner, i.e. without localisation errors.
- When applying the system according to the invention acoustical feedback will be kept to a minimum in that:
- 1. Largely direct sound is picked up; the microphones are positioned principally on and around the source area, as e.g. the stage; acoustical feedback can be further reduced by:
- 2. the use of directive microphones;
- 3. the use of directive loudspeakers - in particularly directed to the audience;
- 4. making the components of the processor time-variable.
- Furthermore the acoustical noise may be reduced by:
- 1. positioning one or more microphones adjacent the acoustical noise sources;
- 2. supplying the microphone signals to the loudspeakers via a multi-channel-anti-noise filter and
- 3. selecting the filter coefficients of the anti-noise filter such that the acoustical noise is compensated at the loudspeakers.
- A major advantage of the system according to the invention is to be seen in that fine-tuning from the real room is possible, as a re suit of which each desired sound field may be almost completely achieved.
- The electro-acoustical system according to the present invention may be realised in eight steps:
- 1. analysis of the aoustical conditions in the real room;
- 2. specification of the desired acoustical conditions - in case of a multi-functional hall also the desired variations relative to a reference-acoustical condition;
- 3. determination of the number and positions of the microphones and loudspeakers;
- 4. building and pre-programming of the system;
- 5. installation of the system;
- 6. fading in of the system, so that the desired referential acoustical condition will be realised ("calibration");
- 7. varying the system parameters, so that, starting from the referential acoustics, a number of preferred presettings may be obtained in accordance with the various purposes ("from reference to preference") and
- 8. storing of the preferred presettings in the memory of the processor, from which such presettings may be called by means of a keyboard
- With the system according to the invention the following system-parameters may be varied for the realisation of the preferred presettings:
- 1. the reverberation times in frequency bands with central frequencies in the audio region;
- 2. the sound pressure levels in those frequency bands;
- 3. the scale factor of the total reverberation characteristics;
- 4. the input-amplification of all the microphones; and
- 5. the output amplification of all of the loudspeakers.
- Each parameter may be varied in steps. The advantage of the above measures is to be seen in that the fading in of the system may be effected in a quick and simple manner and that each objective and subjective demand can be met.
- The system according to the invention may be composed of three parts:
- 1. the pick up sub-system, comprising the microphones with noise-suppressing pre-amplifiers and equalizers;
- 2. the central processor comprising the reflection-simulating units and
- 3. the reproduction sub-system, comprising the loudspeakers with distortion-free final amplifiers.
- The central processor embodies the transfer matrix T and forms the heart of the electro-acoustical system.
- In the central processor each reflection simulating unit is taking care of a weighed and delayed signal between each microphone and each loudspeaker. The various reflection simulating units are internally coupled. The required number of units depends on the size and the form of the room and the required maximum reverberation time.
- The system according to the invention may consist of any combination of four independent modules, viz. a hall module, a stage module, a speech module and a theatre module.
- The functions of the various modules are as follows:
- By means of this module a desired reverberation field may be realised in the hall, tending to maximum "spaciousness". In halls with deep balconies it will often be necessary to use a number of reverberation modules. Early reflections may be additionally amplified or late reflections may be additionally attenuated to improve the 'definition' of music. By means of the system according to the invention it is even possible to have sound decay at two rates, e.g. at first quick and then slow.
- By means of this module the early reflections desired on the stage may be realised, thereby creating optimum combined action conditions for the musicians of an ensemble.
- This module is speech supporting, use being made of one or more PA-microphones (PA = public address). By means of the speech module the direct sound field (reflections of the order zero) may be reconstructed in any spot of the room in a completely natural manner, i.e. keeping the correct localisation and in each frequency band with any desired level.
- This module is speech supporting by adding early reflections without making use of PA-microphones: the direct sound is picked up by a number of microphones over and/or in front of the stage. Reconstruction is taking place as with the speech module.
- The invention will be hereinafter further explained with refe rence to the accompanying drawings.
- Fig. 1 shows in a caricatural manner the different lines of approach of the architect of a hall and of the acoustician;
- fig. 2 illustrates the principle of the system according to the invention, only one microphone-loudspeaker pair being shown;
- fig. 3 is a diagrammatic view of a sound wave field picked up by an array of microphones, and of a sound wave field reconstructed by means of a processor and an array of loudspeakers;
- fig. 4 shows a block diagram of the system according to fig. 2;
- fig. 5 illustrates the composition of the parts of the system according to the invention;
- fig. 6 shows in diagrammatic form the composition of a reflection simulating unit according to the invention;
- fig. 7 shows the central processor of the system according to the invention;
- fig. 8 illustrates a simulation by means of image sources;
- fig. 9 illustrates the effect of the change of a number of system parameters for the fine-tuning;
- fig. 10 shows a few reverberation times of the aula of the Delft University;
- fig. 11 illustrates a few reverberation times of the York University, Toronto;
- fig.'12 shows a few decay curves of the aula of the Delft University, and
- fig. 13 shows a few decay curves of the York University, Toronto.
- In fig. 1 it has been shown in a simple manner how the
architect 1 comes to a certain shape of the room orhall 2. Theacoustician 3 comes, from his point of view, to a totallydifferent hall shape 4, which is based on acoustical principles. - In practice an optimal cooperation between the
architect 1 and theacoustician 3 will result in a acoustical compromise at the most. - In fig. 2 the principle of the present invention has been shown for one microphone-loudspeaker pair. In i the real architectonic room or
hall 5 the source field is picked up on thestage 6 and transmitted to animpulsive source 13 in a fictive acoustically ideal hall, which is defined in the processor 15 (fig. 3). - In the 'ideal hall' the sound is reverberated. Thereupon the reverberation sound field is picked up by receivers, such as
receiver 8 and transmitted tocorresponding locations 9 in the realarchitectonic room 5 by means of loudspeakers, such asloudspeaker 9.Source 13 in the desiredhall 7 has the same position as themicrophone 6 in thereal room 5. Thereceiver 8 in the desiredhall 7 has the same position as theloudspeaker 9 in thereal hall 5. In this way an acoustically ideal hall may be 'constructed' within the architectonic hall. The acoustical system according to the present invention can be considered to work with two halls: the real hall and a fictive one. - Said one microphone-loudspeaker pair in fig. 2 only serves to illustrate the transfer action or - processing, which is taking place between a microphone and a loudspeaker via reproduction - and pick up components in the fictive hall. In reality the type of transfer aimed at by the invention required a dense network of microphones and loudspeakers, so that a wave field may be created both on the input and the output side. It has been found that by means of linear-y arrays of loudspeakers at the side walls and ceilings with a mutual spacing of about 2 m very good results may be obtained.
- In this connection reference is made to fig. 3, which illustrates how the sound pressure of a propagating wave field is 'measured' by an array of microphones, positioned in plane x = xi. In the generalised version of acoustical holography the measured microphone signals are supplied to a processor which causes the propagation (extrapolation) to an other plane, e.g. x = X2 to take place in a numerical way. With reference to fig. 3 it will be easily understood that the 'measuring result' in plane x = x, may be - as an intermediary step - stored on e.g. an M-track recording tape or similar storage member, which may be played via the processor on any desired moment.
- Fig. 4 illustrates the system according to the invention in block diagram for one microphone-loudspeaker pair. It is to be remarked that the
processor 15 may operate either in the analog or in the digital mode. Theprocessor 15 comprises a reflection-simulator 16 and aconvolver 17 for the convolution processing. If r mn ( t ) represents the impulse response at receiver position n due to impulsive source m, the superscript + indicating that only waves leaving the wall are considered, then the desired reflection patterns at wall position n of the real hall is given by the convolution Pmn (t) = Sm (t) * rmn (t), wherein Sm (t) represents the microphone signal of the direct sound in position m. In the real hall 5 a portion of the response Pmn, however, will be fed back to microphone m. - If said feedback between loudspeaker n and microphone m are not to be neglected the convolution Sm -(t) * r mn ( t) has to be substituted by Sm (t) * r'mn (t) where in the frequency domain (ω)
- 5 Note the fundamental difference between Rmn (ω) and G (ω):
- Rmn (ω) is a simulated transfer function in the desired hall;
- Gnm (ω) is a measured transfer function in the real hall.
- In the system according to the invention the feedback phenomenon (quantified by Gnm) may be minimized, viz. to |Gnm (ω) Rmn (ω)|«1 for all m and n by taking the following measures:
- 1) The loudspeakers direct their energy to the absorbtive area as much as possible.
- 2) The microphones have maximum sensitivity in the direction of the source area and no sensitivity in the opposite direction (Gnm-G) m ).
- 3) The microphones are mounted near the source area where the direct sound level dominates the reverberant sound level.
- 4) The parameters of the desired impulse response Rmn (ω) are made time variable.
- Hence in the system according to the invention Rm n (ω)≈Rmn (ω) is aimed at.
-
- in fig. 5 the data flow has been shown in diagrammatic form. In the system according to the present invention the source wave field is picked up by a network of
microphones 20. Thereupon the desired reflection pattern - belonging to the fictive hall 7 - is simulated by the central processor T. Said reflection pattern is then transmitted to thereal hall 5 by means of a network ofloudspeakers 10. - In fig. 5 (as well as in fig. 7) three stages are to be distinguished:
- I Acquisition
- II Extrapolation
- III Reconstruction
- which stages are embodied in as many sub-systems.
- I. The acquisition sub-system measures the direct sound field with an array of high quality braod- band microphones adjacent the stage. The microphone signals are amplified, optionally equalized and supplied to the extrapolation sub-system.
- II. The extrapolation sub-system consists of a number of reflection simulating units. Depending on the maximum T 60 required and the size of the hall, many reflection simulating units may be needed to include the necessary high-order reflections in Rmn (t).
- III. The reconstruction sub-system transmits the simulating reflections back into the hall by means of an array of high quality broad-band loudspeakers, distributed along the surfaces of the entire hall. It should be noted that at a given position in the hall the reflection tail is not made by just one loudspeaker, but is synthesized by contributions of all of the loudspeakers: holography is principally multi-channel.
- Fig. 6 shows a diagrammatic configuration of a reflection-simulating unit 16 (order zero for speech, first and higher order for reverberation). The coefficients are determined in the manner indicated above.
- In fig. 7 a diagrammatic arrangement of the electro-acoustical system of the invention is shown. The central processor T comprises a number of
reflection simulating units 16. Each reflection simulating unit is determined by the transfer function between Msources 11 andN loudspeakers 12 for a certain order of reflection. - If the M input signals of the extrapolation sub-system in fig. 5 or7 are represented by input factor S ("source") and the M output signals are indicated by output factor P ("pressure"), the relation between input and output may be represented by a transfer matrix T ("transfer") as follows:
- where i is the number of reflections against the side walls;
- j is the number of reflections against front and back walls and
- k is the number of reflections against ceiling and floor.
- The source factor S is composed of a number of sub-factors S ;jk.
- Fig. 8 illustrates the simulation of the desired reverberation field, by using the image source approach. Each simulating unit represents the transfer function between the sources in one image version of the fictive hall and the loudspeaker in the real hall.
- Tijk thus represents the transfer function between the M sources in the fictive (i, j, k) and the relevant loudspeaker in the real hall. If the floor is considered to be fully absorptive then k = 0 or 1. If the back wall is considered to be fully absorptive, then j = 0 or 1. For direct sound control i = 0, j = 0 and k = 0.(fig. 6).
- After the system according to the invention has been installed the fine-tuning procedure may start. The principle of it is as follows: at first a reference setting is determined by carrying out interactive measurements such that T so values and sound pressure levels meet the specifications. The reference setting could be selected such that, when the system is switched on, the reverberation time values in octave bands measured in the hall correspond to those in the Amsterdam Concertgebouw, with reverberant sound pressure levels related to the reverberation times according to physical laws. As mentioned before, appropriate ratios of early-to-late and lateral-to-frontal energy could be aimed at.
- Starting from the reference setting, that is stored in the memory of the processor of the system, preference settings can be adjusted to 'instantaneous multi-purpose requirements' or 'subjective alternatives' by varying 19 fine-tuning parameters:
- 1 - 8 : the individual reverberation time values in the 8 octave bands from 63 Hz up to 8 kHz;
- 9 - 16 : the individual pressure levels in the same octave bands;
- 17 : the scaling factor for all reverberation times;
- 18 : the input amplification of all microphones:
- 19 : the output amplification of all loudspeakers.
- In fig. 10 and 11 a few reverberation times are indicated, which apply for auditorium of the Delft University and for the York University (Toronto) respectively, without and with the system according to the present invention.
- Fig. 12 and 13 show a few decay curves, applying for the auditorium of the Delft University ('single decay') and the York University ('double decay') respectively for 500 Hz. It will be appreciated, that very small decay rates may be generated without the slightest tendency to colouring. It has been found that settings with relatively strong early reflections (or relatively weak late-reflections) create an excellent intelligibility, even with reverberation times of as high as 4s.
Claims (7)
1. A method for processing the sound emitted by one or more sound sources in a listening room, by recording said sound by means of a number of microphones, the signals (S) of which are processed in a processor according to the matrix relation P = T S , in which (P) represents the processed signals supplied from the processor to a number of loudspeaker distributed across the listening room, and wherein T represents the following transfer matrix: wherein M and N represent the number of microphone signals and loudspeaker signals respectively, characterized in that the microphone array is arranged to pick up the wave field of the direct sound originating from all of the sources on the stage, the elements of the matrix T being selected according to the Green's function in the Kirchhoff-integral for two dimensions, and for three dimensions, where rnm = the distance between microphone m and loudspeaker n, after which processing the loudspeaker array will, with a correct loudspeaker spacing, generate a wave field, that approaches a natural sound field in an acoustically ideal hall.
2. A method according to claim 1, characterized in that sound wave fields which are (additionally) based on (very) early end/or late reflections (reverberant sound) may be simulated by (additionally) processing the picked up direct sound signals according to the matrix relation where S ijk represent the image sources in the acoustically desired image hall (i, j, k) and Tijk represent the Kirchhoff-based transfer matrix of the image sources in the image hall (i, j, k) to the loudspeakers in the real listening room and where for the image sources S ijk = (1 - αijk) S applies, where αijk represents the total absorption after (i + j + k) reflections.
3. A method according to claims 1 - 2, characterized in that the microphone (signals) are stored on a recording means prior to being supplied to the processor.
4. Electro-acoustical system for picking up the sound emitted by one or more sound sources on a stage in a listening room by means of an array of microphones, which are connected to a processor, the outputs of which are connected to an array of loudspeakers distributed accross the listening room, the processor being designed to create between the micro signals S and the loudspeaker signals P the transfer matrix relation: wherein M and N represent the number of microphone signals and loudspeaker signals respectively, characterized in that the microphone array is arranged to pick up the wave field of the direct sound originating from all of the sources on the stage, the elements of the matrix T being selected according to the Green's function in the Kirchhoff-integral for two dimensions, and for three dimensions, where rnm = the distance between microphone m and loudspeaker n, after which processing the loudspeaker array will, with a correct loudspeaker spacing, generate a wave field, that approaches a natural sound field in an acoustically ideal hall.
5. Electro-acoustical system according to claim 4, characterized in that the processor is also designed to process the (largely) direct sound picked up by the microphones according to the matrix relation where S ijk represent the image sources in the acoustically desired image hall (i, j, k) and Tijk represent the Kirchhoff-based transfer matrix of the image sources in the image hall (i, j, k) to the loudspeakers in the real listening room and where for the image sources S ijk = (1 - αijk) S applies, where αijk represents the total absorption after (i + j + k) reflections.
6. Electro-acoustical system according to either of claims 4-5, characterized in that the processor is designed to modify the transfer function Rm" (ω) between microphone m and loudspeaker n according to where Gnm (ω) represent the transfer function of the real hall between loudspeaker n and microphone m.
7. Electro-acoustical system according to claims 4 - 6, characterized by a compensation circuit with an anti-noise filter satisfying the relation where I represents the microphone position adjacent an acoustical noise source, if any, and Fln (ω) represents the desired transfer function of the anti-noise filter between microphone I and loudspeaker n, said compensation circuit being adapted to be selectively switched on.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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NL8800745 | 1988-03-24 | ||
NL8800745A NL8800745A (en) | 1988-03-24 | 1988-03-24 | METHOD AND APPARATUS FOR CREATING A VARIABLE ACOUSTICS IN A ROOM |
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EP0335468A1 true EP0335468A1 (en) | 1989-10-04 |
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ID=19851997
Family Applications (1)
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EP89200785A Withdrawn EP0335468A1 (en) | 1988-03-24 | 1989-03-28 | Electro-acoustical system |
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US (1) | US5142586A (en) |
EP (1) | EP0335468A1 (en) |
JP (1) | JPH02503721A (en) |
AU (1) | AU630094B2 (en) |
CA (1) | CA1319891C (en) |
NL (1) | NL8800745A (en) |
NO (1) | NO175838C (en) |
WO (1) | WO1989009465A1 (en) |
ZA (1) | ZA892274B (en) |
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Also Published As
Publication number | Publication date |
---|---|
NL8800745A (en) | 1989-10-16 |
US5142586A (en) | 1992-08-25 |
NO175838B (en) | 1994-09-05 |
NO894666L (en) | 1990-01-23 |
WO1989009465A1 (en) | 1989-10-05 |
AU3431589A (en) | 1989-10-16 |
NO175838C (en) | 1994-12-14 |
JPH02503721A (en) | 1990-11-01 |
CA1319891C (en) | 1993-07-06 |
AU630094B2 (en) | 1992-10-22 |
ZA892274B (en) | 1989-11-29 |
NO894666D0 (en) | 1989-11-23 |
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